2017
DOI: 10.1364/optica.4.000736
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Further improvements to the ptychographical iterative engine

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Cited by 347 publications
(215 citation statements)
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“…As a result, both A ν A † ν and B g B † g are Hermitian symmetric and hence define orthogonal projections for any ν and g. By the asymptotic (1 + ) λ(1+ )+1/2 ∼ e λ +λ 2 /2 we have P (n) ∼ e −λ 2 /2 √ 2πλ = e −(n−λ) 2 /(2λ) √ 2πλ . (91) 31 Namely in the low noise limit the Poisson noise is equivalent to the Gaussian noise of the mean |Af | 2 and the variance equal to the intensity of the diffraction pattern. The overall SNR can be tuned by varying the signal energy Af 2 .…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…As a result, both A ν A † ν and B g B † g are Hermitian symmetric and hence define orthogonal projections for any ν and g. By the asymptotic (1 + ) λ(1+ )+1/2 ∼ e λ +λ 2 /2 we have P (n) ∼ e −λ 2 /2 √ 2πλ = e −(n−λ) 2 /(2λ) √ 2πλ . (91) 31 Namely in the low noise limit the Poisson noise is equivalent to the Gaussian noise of the mean |Af | 2 and the variance equal to the intensity of the diffraction pattern. The overall SNR can be tuned by varying the signal energy Af 2 .…”
Section: Resultsmentioning
confidence: 99%
“…We see that the Gaussian-DRS outperforms the Poisson-DRS, especially when the Poisson RE becomes unstable for NSR ≥ 35%. As noted in [10,31,50] fast convergence (with the Poisson log-likelihood function) may introduce noisy artifacts and reduce reconstruction quality.…”
Section: Test Objectsmentioning
confidence: 99%
“…The multi-slice ptychography reconstruction was conducted using 1000 iterations of the regularized ptychographic iterative engine (Maiden et al, 2017). The probe function propagated from the wavefront reconstructed from the single-slice dataset was used as the starting guess for the probe on the front slice.…”
Section: Resultsmentioning
confidence: 99%
“…The wavefront exiting the last slice carries the depth information of the entire sample and propagates to the detector plane. The recorded far-field diffraction pattern is used to update the wavefront exiting from the last slice, where the probe and the object functions are decoupled using conventional ptychographic algorithms (Maiden & Rodenburg, 2009;Maiden et al, 2017). The obtained probe function is then sequentially back-propagated to the previous slices, and updates the corresponding probe and object functions on each slice.…”
Section: Introductionmentioning
confidence: 99%
“…Among the diverse techniques one method seems to be particularly popular among practitioners. In the physics literature this method is known as the Ptychographic Interative Engine (PIE), and is regarded as a standard approach for image formation from ptychographic data within the physics community [7,8]. Mathematically this approach is an alternating projection method which goes back to the work of Gerchberg and Saxton [9] and Fienup [10].…”
Section: Introductionmentioning
confidence: 99%